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solution manual for Signals and Systems A Primer with MATLAB® 2nd edition by Sadiku

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This document contains the complete solution manual for Signal ProcesThis solution manual provides detailed, step-by-step answers to problems from Signals and Systems: A Primer with MATLAB® (2nd Edition) by Matthew N. O. Sadiku. It covers essential topics such as continuous and discrete-time signals, Fourier series, Fourier transform, Laplace transform, Z-transform, convolution, system properties, and MATLAB applications. Designed for students and instructors in electrical and computer engineering, this manual helps reinforce concepts through solved exercises, making it an essential resource for mastering signals and systems with practical MATLAB and Linear Systems, 2nd Edition by B. P. Lathi. It provides detailed, step-by-step solutions to exercises and end-of-chapter problems, covering both continuous-time and discrete-time signal analysis. Topics include Fourier series and transforms, Laplace transforms, Z-transforms, convolution, sampling, modulation, filter design, and system stability. This manual is an essential study companion for electrical and electronics engineering students, supporting problem-solving practice and exam preparation.

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solution manual for Signals and Systems A Primer with
MATLAB® 2nd edition by Sadiku




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, 3




Table of Contents
Chapter 1 1
Chapter 2 41
Chapter 3 77
Chapter 4 117
Chapter 5 144
Chapter 6 182
Chapter 7 205




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, 4

CHAPTER 1

P. P. 1.1
2 2
The period is T = = =1
 2
x(t + T ) = A cos((2 (t +1) + 0.1 )
= A cos(2 t + 2 + 0.1 )
= A cos(2 t + 0.1 )
= x(t)
Hence x(t) is periodic.

P.P. 1.2

(a) x(t) = t, 0 < t < 
T /2 T /2  T / 2 3
E = lim
T →
 T →

| x(t) |2dt = limt 2
dt = lim 2   =
−T / 2 −T / 2 T →  3 

1
 | x(t) |2dt = lim 1  t 2dt = lim 2  T / 2  = 
T / 2 T / 2 3
P = lim
T → T T → T T → T  3 
−T / 2 −T / 2



i.e. x(t) is neither an energy nor a power signal.

(b)
T /2 a
E = lim  | x(t) |2dt = lim  A dt = 2aA
2 2
T → T →
−T / 2 −a


i.e. x(t) is an energy signal.

(c) | x(n) |= 5 | e− j4n |= 5
 | x[n] |2 = lim  52
N N
1 1
P = lim
N → 2N +1 N → 2N +1
n=− N n=− N
1
= lim 25(2N +1) = 25 
N → 2N +1



i.e x[n] is a power signal.

P.P. 1.3
(a) ze = t 2 −10, zo = 4t




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, 5

1
h (t) = [u(t +1) −u(t −1)]
8s

s8 s8 s8 s8 s8 s8 s8

e 2
(b)
1
h (t) = [−u(t +1) + 2u(t) −u(t −1)]
s8

s 8 s8 s8 s8 s8 s8 s8 8s s8

o
2

These are sketched below. s8 s8 s8 ho
he

½ 1/2



t -1 0 1 t
-1 0 1
-1/2


P. P. 1.4
s8 s8



= sin( / 2) =1
(a)
−
sin(t3 + /2)(t)dt =sin(t3 + /2)
s8
s8 8s s8 s8
8s
s8 s8 s8 s8 8s s8 s8

t =0 s8 s8
s8 s8 s8 s8 8s




10

=1 + 4 − 2 = 3

(b) (t2 + 4t − 2)(t −1)dt = (t2 + 4t − 2)
0
8s
8s s8 s8 s8 s8 s8 s8 s8 s8 8s s8 s8 s8 s8

t =1s8 8s
8s s8 8s s8 s8 s8




P. P. 1.5
s8 s8



 0, t 0
 s8 s8




i(t) =  10, s8 s8
s8
0t  2s8 s8 s8 s8




 −10, 2t  4 s8 s8 s8 s8




i(t) =10u(t) −u(t − 2)−10u(t − 2) −u(t − 4)
s8 8s s8 s8 s8 s8 8s s8 s8 s8 s8 s8 s8




=10[u(t)− 2u(t − 2) +u(t − 4)]
8s s8 s8 s8 s8 s8 s8 s8 s8




t

Let I = s8 s 8


−
idt s8




For t < 0, s 8 s8 s8 s 8 I = 0. s8 s8


t

For 0 < t < 2, I = 10dt =10t
s8 s8 s 8 s8 s8 s8 s8 s8 8s


0
2 t
t
For 2 < t < 4,
s8 s8 s8 s8 s8
I = 10dt − 10dt = 20−10t
s8 s8 s8 s8 s8 s8 8s = 40−10t
s8 8s


0 2
2
4
For t > 4, s 8 s8 s8
I = 20−10ts8 s8 s8 =0 s8


2
Thus,
s8




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Matthew N. O. Sadiku, Warsame Hassan Ali, Sarhan M. Musa Signals and Systems
Publisher: 2024 ISBN: 9781040045879 Edition: Unknown

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